9 research outputs found

    Helical multistage isotope separator

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    CELLDEX2018

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    Data and code associated with the manuscript: SD Tiegs, DM Costello, MW Isken, G Woodward, PB McIntyre, MO Gessner, E Chauvet, NA Griffiths, AS Flecker, et al. Global patterns and drivers of ecosystem functioning in rivers and riparian zones

    Asteroid Measurements at Millimeter Wavelengths with the South Pole Telescope

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    International audienceAbstract We present the first measurements of asteroids in millimeter wavelength data from the South Pole Telescope (SPT), which is used primarily to study the cosmic microwave background (CMB). We analyze maps of two ∌270 deg2 sky regions near the ecliptic plane, each observed with the SPTpol camera ∌100 times over 1 month. We subtract the mean of all maps of a given field, removing static sky signal, and then average the mean-subtracted maps at known asteroid locations. We detect three asteroids—(324) Bamberga, (13) Egeria, and (22) Kalliope—with signal-to-noise ratios (S/N) of 11.2, 10.4, and 6.1, respectively, at 2.0 mm (150 GHz); we also detect (324) Bamberga with an S/N of 4.1 at 3.2 mm (95 GHz). We place constraints on these asteroids’ effective emissivities, brightness temperatures, and light-curve modulation amplitude. Our flux density measurements of (324) Bamberga and (13) Egeria roughly agree with predictions, while our measurements of (22) Kalliope suggest lower flux, corresponding to effective emissivities of 0.64 ± 0.11 at 2.0 and &lt; 0.47 at 3.2 mm. We predict the asteroids detectable in other SPT data sets and find good agreement with detections of (772) Tanete and (1093) Freda in recent data from the SPT-3G camera, which has ∌10× the mapping speed of SPTpol. This work is the first focused analysis of asteroids in data from CMB surveys, and it demonstrates we can repurpose historic and future data sets for asteroid studies. Future SPT measurements can help constrain the distribution of surface properties over a larger asteroid population.</jats:p

    SPT Clusters with DES and HST Weak Lensing. II. Cosmological Constraints from the Abundance of Massive Halos

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    International audienceWe present cosmological constraints from the abundance of galaxy clusters selected via the thermal Sunyaev-Zel'dovich (SZ) effect in South Pole Telescope (SPT) data with a simultaneous mass calibration using weak gravitational lensing data from the Dark Energy Survey (DES) and the Hubble Space Telescope (HST). The cluster sample is constructed from the combined SPT-SZ, SPTpol ECS, and SPTpol 500d surveys, and comprises 1,005 confirmed clusters in the redshift range 0.25−1.780.25-1.78 over a total sky area of 5,200 deg2^2. We use DES Year 3 weak-lensing data for 688 clusters with redshifts z<0.95z<0.95 and HST weak-lensing data for 39 clusters with 0.6<z<1.70.6<z<1.7. The weak-lensing measurements enable robust mass measurements of sample clusters and allow us to empirically constrain the SZ observable--mass relation. For a flat Λ\LambdaCDM cosmology, and marginalizing over the sum of massive neutrinos, we measure Ωm=0.286±0.032\Omega_\mathrm{m}=0.286\pm0.032, σ8=0.817±0.026\sigma_8=0.817\pm0.026, and the parameter combination σ8 (Ωm/0.3)0.25=0.805±0.016\sigma_8\,(\Omega_\mathrm{m}/0.3)^{0.25}=0.805\pm0.016. Our measurement of S8â‰ĄÏƒ8 Ωm/0.3=0.795±0.029S_8\equiv\sigma_8\,\sqrt{\Omega_\mathrm{m}/0.3}=0.795\pm0.029 and the constraint from Planck CMB anisotropies (2018 TT,TE,EE+lowE) differ by 1.1σ1.1\sigma. In combination with that Planck dataset, we place a 95% upper limit on the sum of neutrino masses ∑mÎœ<0.18\sum m_\nu<0.18 eV. When additionally allowing the dark energy equation of state parameter ww to vary, we obtain w=−1.45±0.31w=-1.45\pm0.31 from our cluster-based analysis. In combination with Planck data, we measure w=−1.34−0.15+0.22w=-1.34^{+0.22}_{-0.15}, or a 2.2σ2.2\sigma difference with a cosmological constant. We use the cluster abundance to measure σ8\sigma_8 in five redshift bins between 0.25 and 1.8, and we find the results to be consistent with structure growth as predicted by the Λ\LambdaCDM model fit to Planck primary CMB data

    SPT Clusters with DES and HST Weak Lensing. II. Cosmological Constraints from the Abundance of Massive Halos

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    International audienceWe present cosmological constraints from the abundance of galaxy clusters selected via the thermal Sunyaev-Zel'dovich (SZ) effect in South Pole Telescope (SPT) data with a simultaneous mass calibration using weak gravitational lensing data from the Dark Energy Survey (DES) and the Hubble Space Telescope (HST). The cluster sample is constructed from the combined SPT-SZ, SPTpol ECS, and SPTpol 500d surveys, and comprises 1,005 confirmed clusters in the redshift range 0.25−1.780.25-1.78 over a total sky area of 5,200 deg2^2. We use DES Year 3 weak-lensing data for 688 clusters with redshifts z<0.95z<0.95 and HST weak-lensing data for 39 clusters with 0.6<z<1.70.6<z<1.7. The weak-lensing measurements enable robust mass measurements of sample clusters and allow us to empirically constrain the SZ observable--mass relation. For a flat Λ\LambdaCDM cosmology, and marginalizing over the sum of massive neutrinos, we measure Ωm=0.286±0.032\Omega_\mathrm{m}=0.286\pm0.032, σ8=0.817±0.026\sigma_8=0.817\pm0.026, and the parameter combination σ8 (Ωm/0.3)0.25=0.805±0.016\sigma_8\,(\Omega_\mathrm{m}/0.3)^{0.25}=0.805\pm0.016. Our measurement of S8â‰ĄÏƒ8 Ωm/0.3=0.795±0.029S_8\equiv\sigma_8\,\sqrt{\Omega_\mathrm{m}/0.3}=0.795\pm0.029 and the constraint from Planck CMB anisotropies (2018 TT,TE,EE+lowE) differ by 1.1σ1.1\sigma. In combination with that Planck dataset, we place a 95% upper limit on the sum of neutrino masses ∑mÎœ<0.18\sum m_\nu<0.18 eV. When additionally allowing the dark energy equation of state parameter ww to vary, we obtain w=−1.45±0.31w=-1.45\pm0.31 from our cluster-based analysis. In combination with Planck data, we measure w=−1.34−0.15+0.22w=-1.34^{+0.22}_{-0.15}, or a 2.2σ2.2\sigma difference with a cosmological constant. We use the cluster abundance to measure σ8\sigma_8 in five redshift bins between 0.25 and 1.8, and we find the results to be consistent with structure growth as predicted by the Λ\LambdaCDM model fit to Planck primary CMB data

    SPT Clusters with DES and HST Weak Lensing. II. Cosmological Constraints from the Abundance of Massive Halos

    No full text
    International audienceWe present cosmological constraints from the abundance of galaxy clusters selected via the thermal Sunyaev-Zel'dovich (SZ) effect in South Pole Telescope (SPT) data with a simultaneous mass calibration using weak gravitational lensing data from the Dark Energy Survey (DES) and the Hubble Space Telescope (HST). The cluster sample is constructed from the combined SPT-SZ, SPTpol ECS, and SPTpol 500d surveys, and comprises 1,005 confirmed clusters in the redshift range 0.25−1.780.25-1.78 over a total sky area of 5,200 deg2^2. We use DES Year 3 weak-lensing data for 688 clusters with redshifts z<0.95z<0.95 and HST weak-lensing data for 39 clusters with 0.6<z<1.70.6<z<1.7. The weak-lensing measurements enable robust mass measurements of sample clusters and allow us to empirically constrain the SZ observable--mass relation. For a flat Λ\LambdaCDM cosmology, and marginalizing over the sum of massive neutrinos, we measure Ωm=0.286±0.032\Omega_\mathrm{m}=0.286\pm0.032, σ8=0.817±0.026\sigma_8=0.817\pm0.026, and the parameter combination σ8 (Ωm/0.3)0.25=0.805±0.016\sigma_8\,(\Omega_\mathrm{m}/0.3)^{0.25}=0.805\pm0.016. Our measurement of S8â‰ĄÏƒ8 Ωm/0.3=0.795±0.029S_8\equiv\sigma_8\,\sqrt{\Omega_\mathrm{m}/0.3}=0.795\pm0.029 and the constraint from Planck CMB anisotropies (2018 TT,TE,EE+lowE) differ by 1.1σ1.1\sigma. In combination with that Planck dataset, we place a 95% upper limit on the sum of neutrino masses ∑mÎœ<0.18\sum m_\nu<0.18 eV. When additionally allowing the dark energy equation of state parameter ww to vary, we obtain w=−1.45±0.31w=-1.45\pm0.31 from our cluster-based analysis. In combination with Planck data, we measure w=−1.34−0.15+0.22w=-1.34^{+0.22}_{-0.15}, or a 2.2σ2.2\sigma difference with a cosmological constant. We use the cluster abundance to measure σ8\sigma_8 in five redshift bins between 0.25 and 1.8, and we find the results to be consistent with structure growth as predicted by the Λ\LambdaCDM model fit to Planck primary CMB data
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